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Bulk modulus measures resistance of Continuum body to compression/decompression and to deformation and is inverse to Compressibility compressibility 

LaTeX Math Inline
bodyc
:

LaTeX Math Block
anchorc
alignmentleft
K = \frac{1}{c}


Bulk modulus depends on the thermodynamic conditions at which it is measured and as such is not a material property.

The two major deformation processes of the medium compression/decompression processes are isothermal and isentropic which result in different values of Bulk modulus:

Isothermal bulk modulusIsentropic Compressibilitybulk modulus

LaTeX Math Inline
bodyT = \rm const

LaTeX Math Inline
bodyS = \rm const

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anchorcT
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K_T = \rho \cdot \left( \frac{\partial p}{\partial \rho} \right)_T
LaTeX Math Block
anchorcS
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K_S = \rho \cdot \left( \frac{\partial p}{\partial \rho} \right)_S

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Both 

LaTeX Math Inline
bodyK_T
 and 
LaTeX Math Inline
bodyK_S
 are not dependent on the amount of chemical substance and defined under a clear specific conditions of thermodynamic process and 
as such are the material properties and properly tabulated for the vast majority of materials.

In engineering practise, when the term Bulk modulus is used as material property it normally means Isothermal Compressibility

LaTeX Math Inline
bodyK=K_T
.

For isotropic materials it is related to Young modulus (E) and Poisson's ratio (ν) as:

LaTeX Math Block
anchorKE
alignmentleft
K_T = \frac{E}{3 \, (1- 2\, \nu)}


See also

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Physics / Mechanics /  Continuum mechanics Continuum mechanicsBody / Deformation

Solid Mechanics  Continuum body] [ Fluid Mechanics]

[Compressibility] [ Young modulus (E) ]Poisson's ratio (ν) ]

Isothermal Compressibility ][ Isentropic Compressibility ]

[Fluid compressibility] [Pore compressibility] [Total compressibility]Compressibility (β or c)]